Electro-mechanical device



April l0, 1962 w. w. MOE

ELECTRO-MECHANICAL DEVICE 8 Sheets-Sheet 1 Original Filed Sept. 3, 1953 mm1 lm mul INVENTOR WI LIAM WEST MOE ATTORNEY April 10, 1962 w. w. MOE

ELECTRO-MECHANICAL DEVICE Original Filed Sept. 5, 1953 8 Sheets-Sheet 2 aw Flsa INVENTOR.

WILLIAM WEST MOE FIG. 4

BY l 74ML, ZM/6 ATTORNEY April 10, 1962 W. W. MOE

ELECTRO-MECHANICAL DEVICE Original Filed Sept. 3, 1955 fai T FIG. 5 ,.,A `\f5' 52-` 66a 67% Flcsd I l l 66% m 5,5 Flash A* f im FIG e 67% f c Z j( 65@ -652/ 672! {664 F|G-6d I l 67;/ IW- 6 Flee 65 l l`70? 665C f, f Fleer 67f 7/f\ g l 70? l ffy-fr 66'? Flsg i 7,?*3P 74f724. l l l F INVVENTOA 73 WILLIAM wsT MoE BY l /LLL/ n ATTORNEY April 10, 1962 w. w. MOE 3,029,387

ELECTRO-MECHANICAL DEVICE Original Filed Sept. 3, 1953 8 Sheets-Sheet 4 /63 //afalzz'/l/f/P JNVENTOR.

2 WILLIAM WEST MOE ATTORNEY April l0, 1962 -MECHANICAL DEVICE 8 Sheets-Sheet 5 Original Filed Sept. 3, 1953 INVENTOR.

ATTORNEY April l0, 1962 w. w. MOE

ELECTRO-MECHANICAL DEVICE 8 Sheets-Sheet 6 Original Fil-ed Sept. 3, 1953 56 4 4 2 a 22]* m 43. 2 me |06.. 2 .3

ATTORNEY April 10, 1962 w. w. MOE

ELECTRO-MECHANICAL DEVICE 8 Sheets-Sheet '7 Original Filed Sept. 3, 1953 ill.

WILLIAM WEST MOE April 10, 1962 w. w. MOE 3,029,387

ELECTRO-MECHANICAL DEVICE Original Filed Sept. 3, 1953 8 Sheets-Sheet 8 Ww (am,

ATTORNEY United States Patent() 3,029,387 ELECTRO-MECHANICAL DEVICE William West Moe, Stratford, Conn., assignor to Time, Ilcorporated, New York, N.Y., a corporation of New Original application Sept. 3, 1953, Ser. No. 378,294, nowv Patent No. 2,865,984, dated Dec. 23, 1958. Divided and this application July 15, 1958, Ser. No. 748,629

3 Claims. (Cl. 324-97) The present invention relates generally to visual image transference apparatus adapted to convert intelligence embodied in an original visual subject into electric signals for subsequent conversion in turn into a replica ofthe visual original. More particularly, the present invention relates to new and improved systems of the above noted character in which provision is made to minimize loss of edge sharpness of the image between scanning of the visual original and the eventual reproduction of the replica thereof.

This application is a division of my eo-pending application, Serial No. 378,294, tiled September 3, 1953, now Patent No. 2,865,984.

In visual image transference systems of the type described, during image transference loss of sharpness tends to occur for regions of the scanned visual subject corresponding to an edge, or sharp change in tone density between adjoining areas of the subject. One factor contributing to this loss in sharpness concerns the electro-optical scanners used as the front end of such systems. In such scanners the scanning aperture, being of finite size, often has a larger diameter than therwidth of the edge between relatively light and dark areas of the scanned original. It follows that when an edge is in the visual tield of the aperture, the light passed by the aperture derives from both the light and dark areas to be associated in an admixture which is irresolvable to the employed light receiving element (as, for example, a photocell). Hence, as long as the edge is in the aperture eld, the photocell produces a signal representing as to tone density, neither a light area nor a dark area, but instead a tone intermediate the tWO.

Since the edge is Viewed by the aperture for a scanning travel thereof equal to the aperture diameter, the photocell produces the mentioned intermediate tone signal for the entire interval required for the aperture to make this travel. Accordingly, the signal generated by the photocell during scanning of an edge does not properly represent the sharp change in tone density of the edge, but represents instead a gradual change in tone density, as would be characteristic of a t-one density transition zone lying ,between a light area and a dark area and having a width equal to the diameter of the scanning aperture.

As to other factors contributing to loss of sharpness of the image, first, an effect similar to that described occurs with regard to the aperture or its equivalent (such as the cathode ray tube beam spot in a television receiver) used to visually reproduce the transmitted image. Second, the nite band width of the image transference system often does not permit of signals having as sharp change in characteristic as the change in tone density at an edge. Third, where a half tone replica is produced, the discontinuous dot characteristic of the half tone surface causes a loss in edge sharpness Accordingly, it is an object of the invention to provide methods and apparatus for overcoming the above noted difficulties in maintaining edge sharpness in visual' image transference systems.

Another object of the invention is to provide methods and apparatus for maintaining edge sharpness between the conversion of the intelligence embodied in an original visual subject into .electric signals, and the reconversion Y by providing, in conjunction with a system which converts the intelligence embodied in a visual subject into electric signals, modifies the signals and then supplies them to an output, a means which, whenever the edge of a visual subject is scanned, superposes at this output a compensating signal upon the image carrying signal of the system. This compensating signal is of a nature to restore the loss of edge sharpness incurred by the image carrying signal in the main channel of the system.

'I he vinvention may be better understood from the following detailed description of a representative embodiment thereof taken in conjunction with the accompanying drawings in which:

FIGURE 1 represents in block diagram form certain portions of an electronic printer apparatus for producing monochrome half-tone negatives or positives from a colored original, and in schematic diagram form the transverse edge-sharpening circuits associated with this apparatus;

FIGURE 2 illustrates a portion of a visual subject having an edge lying transversely across the path of a scanning aperture which travels from a light to a dark area;

FIGURES 3ft-3g, inclusive, illustrate wave forms which indicate for the transverse edge of FIGURE 2 how, by the use of edge correcting signals, edge sharpness may be retained in the course of visual image transference;

FIGURE 4 represents a positive replica of the' portion of thevisual subject shown in FIGURE 2, the replica having a reproduced edge and an edge accentuating zone;

FIGURE 5 illustrates a visual subject portion similar to that shown by FIGURE 2 except that the positions of the light and dark areas are reversed; v

FIGURES 6a-6g, inclusive, illustrate wave forms'of signals derived from the visual subject portion of FIG-A URE 5 but otherwise respectively corresponding to the wave forms of FIGURES 3cr-3g, inclusive; 1

FIGURE 7 illustrates a positive replica of the visual subject portion shown in FIGURE 5, the replica being reproduced from the edge-corrected image carrying signal shown by FIGURE 6g; d i FIGURE 8 represents a portion of a visual subject in which anvedge between a light and a dark area lies parallel to the scanning path traversingy the subject;

FIGURE 9 represents ya plot of the scanning photocell output signals respectively produced during the separate scannings across the visual 'subject portion of FIGURE 8;

FIGURE l0 represents a plot of image carrying signals derived from the output signalsvshown by FIGURE 9, the image carrying signals having applied thereto the necessary signal correction to provide for proper parallel edge reproduction and accentuation; l

FIGURE ll represents a positive replica of the visual subject portion of FIGURE 8, the replica being produced from the corrected image-carrying signals of FIGURE 10;

FIGURE l2 illustrates in diagrammatic form a prescanner optical system which, to provide parallel edge sharpness correction, is adapted to sample the visual eld lon either side of a scanning path taken across a visual subject;

FIGURE I3 represents, in schematic diagram form, circuits adapted, responsive to light energy received by the sampling action of the optical system of FIGURE l2, to produce parallel edge sharpness correction signals;

FIGURES 14a-18a, inclusive, 14bl8b, inclusive, and 14e-18e, inclusive, represent diagrams explanatory of the mode by which parallel edge correction is obtained; i

alpages? FIGURE 19 is a plan view of a high-speed galvanorn-Y eter for driving the sampling mirror in the optical system of FIGURE 12;y

FIGURE 20 is a front elevation of the high-speed galvanorn'eter with a part thereof being shown in cut-away 4 provide edge sharpness restoration through the black channel only.

f `General Description While theinvention may be applied to any visual image transference system, including both black and white and color systems, for purposes of illustration it will be described Iherein in connection with an electronic color printer for producing a plurality of monochrome separation half-tone negatives or positives from a colored original visual subject. The electronic printer to be described is of the so-called four color type utilizing the three sub-Y tractive colors, yellow, magenta'and cyan, and, as a fourth color, black. The details of the printer referred to are fully described in my copending applicationA Serial No. 251,898, tiled October 18, 1951, and entitled High Frequency Carrier System Ifor Electronic Color Correction System, now Patent No. 2,873,312, but to facilitate understanding of the present invention, 'a brief outline is given. below as tor the salient features 'of the printer.

Referring to FIGURE l, the box designates convenient scanning mechanism which may be 'of any suitable type, such as that shown in UnitedStates Patent No. 2,253,086, for example. Itspurpose is to scan elemental areas of a colored original and to provide three electric signals corresponding to the three primary color components in each area scanned. The three output signals for the scanner 30 are `derived from three similar photosen- Sitiye scanning elements 31, 31 vand 31"y (for example, photomultiplier tubes) 'within the scanner 30;

The three scanner output signals so derived from the thi-.ee scanningphototube's 31 31', 31" are fed respectively into three electrical channels which will be designated herein the yellow, magenta and cyan channels, in accord- 'ance with the color of the printing plates produced by the respective channels. Certain elements in each of the three ychannels are identical. Accordingly, when possible, only the yellow channel will be described in detail and corresponding elements in the magenta and cyan channels will be designated by corresponding prime and double prime characters respectively.

In the yellow channel the image-carrying output signal from the scanning phototube 31 is supplied by a lead 35 to a first set of yellowisignal modifying circuits 36. These circuits 36, in operating on the yellow `signal, perform, among vother functions, impression of the output signal from the phototube as a modulation upon a high frequency carrier.

l Continuing to trace the yellow signal through its main channel, the signal flows by a lead 37 from the output ofthe first set of modifying circuits 36 to the input of a second set of yellow'signal modifying circuits 33. Additionally, a signal is supplied from the output of the rst set of modifyingcircuits 36, through an assembly of peak amplitude deriving circuits 39, to a maximum signal selector circuit 40 also receiving signals from the magenta and cyan peak amplitude deriving circuits 39 and 39". The'operations of the peak amplitude deriving circuits and the maximum signal selector circuit are fully explained in the referred to copending application.

The Output signal frornthe maximum signal selector circuit is used tol produce a black separationy negative and also to produce under-colortremoval in essentially'the same manner as described in the copending United States application of William West Moe and Vincent C. Hall, Serial No. 14,008, tiled March 10, 1948 (now United tates- Patent 2,605,348, issued on July 29, 1952, and entitled ColorSeparation Negative).. In the method there disclosed, the black signal st'antaneous maximum modulation component in each of the three channels and the signals in the three channels are reduced as a function of the black signal in order to eect so-called under-color removal.

For under-color removal, the output signal from the maximum signal selector circuit 40 (FIG. l) is supplied as three separate inputs to the three second sets of signal modifying circuits 38, 38', 38f. After performance of additional operations in'these circuits, 'the three image carrying color signals are supplied (with the high fre-r quency carriers eliminated) by respective leads 4d1, 41', and 41 to three respective DC. ampliliers 42, 42 and 42". The outputs of these ampliliers energize three respective glow lamps 43, d3 and 43 which serve to respectively expose the three (yellow, magenta and cyan) photographic emulsions 44, 44 and 44 in the usual manner. Half tone prints may be produced from the photosensitive emulsions in the usual manner.

The output signal from themaximum signal selector circuit 4l) is also supplied to a limiter circuit 45 which may be considered to divert the signal passing therethrough into a black channel. In the black channel the black imagecarrying color signal passes by a lead 46 toa set of circuits 47 adapted to restorel edge sharpness for edges or edge components lying along or parallel to a scanning path. These circuits 47, referred to hereafter as parallel edge circuits, will be later more fully described. From the output of the parallel edge circuits 47 the black image-carrying signal passes by aV lead id-to the input of an amplifier 49. From the output `of the amplifier 49 the image-carrying signal is fed by aleajd 5d to a glow lamp t 531 vadaptedto expose the black print 52.

In operation, the glow lamps 43, 43', 43 and 51 respectively expose four yellow, magenta, cyanv and black color separation half-tone positives or negatives 44, 44', 44 and `52, in synchronismwith the scanning of the colored original visual subject by the scanner 30.

Principle of Transverse Edge Correction As stated, in the electronic color printer described and in other types of visual image transference systems, loss of edge sharpness tends to occur in the system between the yscanning of an original visual subject and the reproduction of a replica or copy of that subject. The factors contributing to this loss in edge sharpness and the cornpensating means therefore will be more clearly understood from a consideration of FIGURES 2, 3a-3g, inclu- Y sive, and 4. As to the mutual relations therebetween, the

mentioned iigures are in vertical registry to have the horizontaldirection of each represent, to a common scale, distance on a scanning path across a visual subject. In the case of FIGURES 3af3g, inclusive, the vertical direction represents the amplitude of an electrical signal.

Referring now to 'FIGURE 2, the figures shows a portion 55 of a visual subject traversed by a scanning aper -ture 56 along a path 57 in the direction indicated by theA arrow 58. 0n the visual subject portion y5S an edge 59, forming a boundary between light and dark areas and 61 of accordingly relatively contrasting tone densityflies across the scanning path 57 in normal relation thereto. Y

Such type edge will be hereafter referred to as a transverse edge, while edges lying along or parallel to, a scanning path will be referred to as"parallel edges. AEdges fitting neither of the above categories will be referred to hereafter as skewed edges.

is derived by selecting the in- Unless otherwise noted,v where the descriptive matter to follow refers to a'transspaces? rence. In order for the output signal from scanningY photocell (say phototube 31 of FIG. l) to accurately signal has a wave form (FIG. 3b), in which a finite slopev transition line 65h connects the high and low signal level regions 6611 and 67b. t

In the course of passing from the output of the photocell through the image transference system circuits, becauseof thel electrical inertia thereof, the signal of FIG. 3b will inevitably be delayed and the slope of the transition line decreased. Hence, atthe output of the mentioned circuits the image carrying signal will have a wave form as in FIG. 3c. In this latter ligure, the signal in wave form no longer represents the sharp change in tone density of an edge but, instead, as shown by line 65e, the gradual change in tone density of a transition zone lying between two areas (shown by lines 66e and 67C) of contrasting tone density.

Theloss in edge sharpness inherent in the wave form of :FIGURE 3c may be electrically compensated for by deriving from the signal of FIGURE 3b a first differential signal (IFIG. 3d). This first differential signal is inverted (FIG. 3e) and differentiated again to produce an inverted second differential signal (FIG. 3f). For edge sharpness correction, this latter signal is superposed on the delayed image-carrying signal (FIG. 3c) at the output of the image-transference system circuits. There results for the image transference system a combined output signal (FIG. 3g).

Considering this combined output signal, note that the edge representing portion thereof, namely transition line 65g, between the high and low signal level regions (66g and 67g) is of considerably increased slope as compared to the transition line 65C of FIGURE 3c. This increased slope in itself is an important factor in reestablishing, as to the image carrying signal, the edge sharpness which would otherwise be lost by the image transference system. In addition, note that in the combined signal (FIG. 3g), the wave form proximate the transition line assumes light and dark tone density peaks 70g and 71g at respectively the light and dark tone ends of the transition line. creation of such contrasting tone peaks, over-accentuating the tone density of the visual subject areas on either side of an edge, is possible for the reason that, in practice very few visual subjects or replicas reproduced therefrom have areas which are completely white or blackr in tone density.

Over-accentuation of edge sharpness, as described, is paritcularly desirable where a visual image transference system is adapted to reproduce half-tone prints from a scanned original. inherently, half-tone prints, because of the discontinuous dots on the surface thereof, tend to suffer from an additional loss of edge sharpness. By over-accentuation, however, this supplementary rloss can be largely corrected to the'eye of a viewer of the halftone print, since the over-accentuated tone density peaks on either side of the true edge position create the optical illustration'that the edge is sharper than in fact it is. Of course, when desirable, over-accentuation can be eliminated by decreasing in a conventional manner the amplitude of the inverted second differential signal (FIG. 3f).

Referring now to FIGURE 4, the figure represents, as a positive replica, the reproduction from the combined signal (FIG. 3g) of the portion 55 of thek original visual subject (FIG. 2). In FIGURE 4, a light tone area 72 and a dark tone area 73 lie to either side of a boundary 74 equivalent toa reproduced edge. Between this boundary 74 and the light area 72 there is present a marginal strip I 75 of lighter tone density than the light area itself. Similarly, between this boundary 74 and the dark area 73 there is present a marginal strip 76 of darker tone density than the dark area itself.

The mentioned light strip 75 andthe dark strip 76, corresponding in the combined signal (FIG. 3g) to the contrasting peaks 70g and 71g on either side of the amplitude transition line, form together an edge accentuating zone '77 coextensive with the position of the edge 59 when shifted slightly in accordance with the signal and 3c.

delay occurring between the waveforms of FIGS.'3b This edge accentuating zone 77 heightens the impression to a viewer of the presence and sharpness ofthe edge, in fact, reproduced.

FIGURES 5, 6a-6g, inclusive, and FIGURE 7 correspond respectively as to subject matter with FIGURES 2, 3ft-3g., inclusive, and 4, with the exception that in the higher numbered group of figures the-scanning aperture" crosses the original edge 59', shown, by moving from a dark area 61 to a light area 69. The corresponding features of the lower and higher .numbered group of figures is indicated by designating corresponding parts in the lower and higher groups with the same number, but with the part number of the lower and higher groups being unprimed and primed respectively. In view of the foregoing description 'as to the mutual relationship between the lowered numbered group of iigures, it is believed that the mutual relations between the higher numbered group of figures is self-explanatory.r

Transverse Edge Correction Circuits Reverting to .FIGURE l, there is shown in schematic form one embodiment of an assemblage of circuits adapted to restore transverse edge sharpness in the manner outlined above. While these transverse edge sharpening circuits are disclosed in detail in the copending application referred to, as a matter of convenience the description of the circuits is also set forth herein. It is to be understood that, unless otherwise noted, the description of the transverse edge sharpening circuits for one color channel of the printer, say the yellow channel, applies as properly to the other printer color channels.

In FIGURE 1, as stated, the yellow channel receives its input from a photosensitive device 31 (such as a conventional photornultipler tube, for example), which forms part of the scanner 30. The photomultiplier tube circuit is arranged so that a negative voltage of, say, -210 volts D.C. is applied to the cathode dynode elements, while the vmultiplier anode is connected by a shielded lead 35 to supply the yellow channel output signal from the scanner 30 to the yellow signal modifying circuits 36.. In the circuits 36, as stated, the signal from the photomultiplier tube 31 is impressed as a modulation upon high frequency carrier.

In order to eliminate capacity loading, a metal cable shield 80 for the Alead 35 is preferably driven in correspondence with the output signals from the photomultiplier tube 31. To this end, the signal upon the lead 35 is fed by a lead 81 to the control grid 82 of a conventional electron tube 83 which is connected in the well known manner to form a cathode follower stage 84. One output of the tube 83 is supplied from the cathode 85 thereof through a resistor 86 and a lead 87 to the sheath 80, a series resonant circuit comprising an inductance 88 and a variable capacitance -89 being connected between the lead 87 and ground to remove from the cable sheath 80 the high frequency carrier signals which may be fed back towardsthe-scanner 30 from the yellow signal modifying circuits 36. As an additional measure for eliminating the high frequency carrier, prefe'rably a condenser 90 is connected between the lead 87 andthe control grid 82 of the tube.

'Since, as stated, sharp edges in the original subject belng scanned may tend to lose some of their sharpnessl in Vtransmission through the multiplicity of electronic circuits comprlsing the printer apparatus heretofore dej 83 at the lead 87 by way of another lead 95 to a differentiating stage 96 incorporating a series condenser 97 and a shunt resistor 98. When in the presence of a Scanned transverse edge the photomultiplier tube 31 pro* duces a signal of the type shown in FIGURE 3b, the condenser 97 and resistor 98 'responsively produce (FIG. 3d) the first differential of the photomultiplier signal.

The first diiierential signal appearingy across the resistor 98 is impressed on the control grid 99 of a conventional electron tube 100 connected in the differentiating stage 96 to act in the usual manner as an amplifier. The first differential signal, ,amplified and inverted (as shown by FIG. 3e), by passage through the tube 100 is taken from the plate 102 of tube 100 and is fed by a conductor 103 to a second difierentiating stage 104 incorporating a series condenser 105 and a shunt resistor 106. The condenser 105V and resistor 106 convert the received inverted first diiierential signal (FIG. 3e) into lthe form of an inverted second differential signal (FIG.

The inverted second difierential signal across resistor 106 is fed to the control grid 110 of an electron tube 111 connected in the differentiating stage 104 as a peaking Voltage amplifier. The output of the tube 111 is taken from the plate 112 thereof and fed by a conductor 113 to`the-D.C. amplifier stage 42.'` In amplifier stage 42 the signal onl conductor 113 is supplied through a blocking condenser 114 to the control grid 11S of an electron Vtube 116 vin the amplifier stage.

The control grid 115 of electron tube 116 receives by way of lead 41 the additional input of the image-carry ing yellow signal lfrom the yellow signal modifying circuits 38. This imagecarrying signal, taken alone, appears at the plate 117 of tube 116- in the form shown by FIG. 3c. Also the inverted second differential signal across resistor 106 undergoes two inversions' by passage through tubes 111 and 116 to appear at the plate 1'17 in the form of FIGURE 3f. Hence, at the output of amplifier stage 42 the inverted second differential signal and the main channel signal are superposed .to produce the combined signal of FIGURE 3g.

As explained, when la visual replica is reproduced vfrom this combined signal through the action of the yellow glow lamp 43 in response thereto, much of the original edge sharpness which is lost in the yellow channel circuits will be restored with regard tothe appearance ofthe replica.

Actually, as stated, it is found desirable in practice to Vso adjust the differentiating `stages `96 and 104 that over-accentuation for the loss of sharpness occurs, i.e., the boundaries between light vand 'dark portions of the picture 'are overdone so that sharpness Lis increased. This tends to compensate for loss of picture edgesV in the halftone printing process. Y

It has' also been found desirable to supply the peaking voltage from the conductor 113' in the magenta channel through a conductor 120 and a condenser 121 to the control grid 1221 of an electron tube 123 in the black printer amplifier 49. By obtaining, as described, the inverted second differential signals from the `photoniultiplier signals in each of the color channels, and iby superposing each inverted second differential signal, on its corresponding delayed image-carrying color signal, the loss of sharpness of transverse edges is largely corrected for. VIn this re` gard, in the case ofthe black channel, itwill be noted that the edge correcting differential signal thereforis derived from a color channel (magenta) otherthan the black channel itself. Thus it is apparent that as to edge vsharpness one color channel may furnish the correcting signal for another. Also, to be noted is the fact thatv as to the black and magenta channels, a single edge correcting `differential signal is used to restore edge sharpness in both of these channels. Thus it is evident that a single edge correcting difierential signal may be used to restore edge sharpness in a plurality of color channels.

Principle of Parallel Edge Correction- Referring to FIGURE Y8, there is shown a portion v' of a scanned visual subject having on its surface an edge 126 forming the boundary between light and dark areas 127 and 12S of relatively contrasting tone density. TheY edge 126 lies parallel to a number of scanning paths a-h inclusive for a scanning aperture 129, the paths being taken across the visual subject portion lin the direction indicated by the arrow heads on the scanning paths. The direction of advance of scan from one scanning path to the next is indicated by the arrow 130 heading a line 1.30ct. l

FIGURE 9 shows as a solid graph line,rthe output of the scanning photocell (for example, the photocell 3jin FIGURE l) as the aperture `129 (FIG. 8) traverses line 130e by one after another of the scanning paths a-h (represented in FIGURE 9 as the vertical `lines a-,h).

Thus, the graph in FIGURE 9 shows the variation .of j scanning photoceli output at line 13011 as the scanning` that the aperture 129 receives light energy from both light` tone andtone areas. Hence, it is evident that a signal response such as is shown in FIGURE 9 represents, for image transfer purposes, a loss in edge sharpness as'the scanning action advances from one side 'to the other of a parallel edge. Y.

In view of the foregoing discussion it isvapparent that restoration of parallel edge sharpness may be obtained,

if to the separate image-carrying signals developed byr the scanning photocell at line 13011 as'shown in FIGURE 9, there is added at appropriate times appropriate parallel edge correcting signals to produce combined signals of conjoint edge restoring effect. The combined signais may be plotted, as shown in FIGURE l0, as a dotted graph line, the horizontal ordinate of the iigure repr eseating, as before, the advance of the scanning action and the vertical ordinate representing, as before, the amplitude of the scanning photocell output. Note that in FIGURE yl0 the graph lines in the iigure as before,

are intersected by a set of vertical lines a`h", inclusive,

representing positionsof advance corresponding to those of scanning paths a-h, inclusive, in FIGURE 8.

By representing in FIGURE l0 the uncorrected imagecarrying signals of FIGURE 9 as a solid graph line, it is apparent that `for earch scanning traverse of the visual subject portion (FIG. S) in a given scanning path,

the amount of correcting signal needed to restore edge sharpness is represented by the vertical distancerbetween the solid and dotted graph lines at Vthe horizontal position representing that scanning path. As in the case of transverse edges, preferably the amplitude of the parallel edge vcorrecting signal is vadjusted for overfaccentuation, in

138 and 139 are created to either side of the transition line 135" between the high and low signal level regions 136 and 137".

The effect of edge correction by the mode described is shown in FIGURE ll, the figure representing a positive replica 1d@ of the visual subject portion 125 of FlGURE 8, the replica being reproduced in accordance with the solid line graph of FGURE 1 0, In FlGURE ll it will be noted that to either side of a boundary 141, representing the true position of the edge 126 on the original subject 125, there are formed tone density accentuated light and dark marginal strips 142 and 143 between, respectively, the boundary 141 and the light and dark areas 1411 and 145. Strips of this type mutually act, as described, to accentuate the tone, density contrast of theoriginal areas. The strips 144 and 14S thus serve to heighten the appearance of an edgeipresence to the' viewer of the replica. Y

i Parallel Edge Optical -.S`yslemv visual subject to be scanned is mounted upon the face ofV a hollow transparent drum 151 adapted rto rotate about a vertical axis. Light originating from a source 152 within the drum is brought by a condensing lens 153 to a focus to form a high intensity light spot 154, the spot being so xedly positioned in space that the transparency d passes through the spot for each rotation of the drum. Concurrent with its rotary motion, the drum 151is advanced in translation upward along its vertical axis in a step-by-step motion. The combined rotary and translatory motions of the drum 151 causes the spot 154 to trace out across the transparency 151B a set of horizontal paths advancing downward successively yfrom one path to the next. Thus, it will be seen that the spot 154in effect causes a scanning action with respect to the visual subject.

The main body of light emanating from the high intensity spot 154 is directed by an objective lens 155 through the aperture of a diaphragm 156, and from thence to the scanner mechanism 30 (FIG. 1). A part of the light passing through the objective lens 155, however, is intercepted by a planar mirror 157 xedly disposed in the center of the optical path and tilted at an angle to deilect the light received thereby to one side of the main optical path.

The light deflected by the planar mirror 157 is directed towards the planar face of a Vibrating mirror 159 adapted to be driven at a speed of 15 kilocycles by a high speed galvanometer assembly 160 to be later described. Vibrating mirror 159 is mounted to sinusoidally oscillate in space about an axis normal to the plane of the drawing. The light received by mirror 159 is reflected therefrom to fall upon the surface of a diaphragm 161 having a small aperture formed therein.

It will be appreciated that, While the entire bundle of light rays reflected by mirrors 157 and 159 and falling upon diaphragm 161 represents an image of au area 161a on transparency 150 considerably exceeding that illuminated by high intensity spot 154, the light passed by the aperture of diaphragm 161 represents, with respect to this image, only a small portion thereof, the portion having the saine order as to size as spot 154. Since the large size image falling upon diaphragm 161 is swept back and forth thereover by the oscillation of mirror 159,

it follows that the portion of image suhtendcd by the aperture of diaphragm 161 represents a small size moving Varea of transparency 150, the small size 'area sweeping as the edge phototube.

10 in a vertical direction and with simple harmonic motion through the high intensity spot 154 as a center.

Thus it may be considered that the aperture of diaphragm 161 defines, in terms of the light passing therethrough, a small auxiliary sampling spot 162 which sinusoidally oscillates in a vertical strip above and below a center position coincident with the main scanning spot 154. In terms of the scanning of transparency 158, therefore, the center of the auxiliary sampling spot 162 may be considered to follow over the transparency a `sinusoidal path symmetrically disposed -about and simultaneously generated with each separate horizontal scanning path generated over the transparency by the main scanning spot 154. This movement, described, of the sampling spot 162 with respect to the transparency 150 results in a continuous sampling of a small width of the visual subject to either side of each horizontal scanning path.

The light passing through the aperture of diaphragm 161 is received by phototube 163, hereafter referred to The light rays so received by the edge phototube 163 are properly focused upon the receiving surface thereof by virtue of the focusing action of the objective lens 155, the focusing effect of which is not affected by reflection of the light rays from the faces of mirrors 157 and 159.

The photocell 163 responsive to the receivedlight energy converts the same into electric signals. Since mirror 159 is driven at a l5 kc. rate, the output signals of photocell 163 will have a l5 kcfundamental frequency along with harmonic components of this frequency.

The Parallel Edge circuits The output signal of the edge photocell 163 is fed by a lead (FIGURES 1 and 13) to the parallel edge circuits section 47 where it is applied to the control grid 171 (FlG. 13) of the triode amplifier 172. The output of triode section 172 is connected through a 30 kc. band pass filter 173 to control grid 174 of another triode section 175 connected in a conventional manner as an amplilier. ln passing through this band pass filter 173, the signal originating with the edge phototube 163 is modified to eliminate the fundamental and all harmonic components thereof except for the second harmonic or 30 kc. component.

The resulting second harmonic signal continues from the output of triode section 175 through two successive amplifying stages consisting of the triode section 176 connected as a conventional amplifier and the triode section 177 connected as a conventional amplifier. At the output of this latter triode section 177 the second harmonic signal excites the primary winding 178 of a transformer 179, the secondary or edge signal winding 150 of which is connected into a polarized rectifier circuit 181. The second harmonic signal is thus coupled over into the polarized rectifier circuit 181.

The parallel edge-circuit section 47 contains, as another component circuit thereof, a triode section connected in a conventional manner as a tuned plate oscillator 186 with a 15 kc. signal. A portion of this l5 kc. signal is extracted as a rst output from the oscillator 186 by a coil 187 inductively coupled to the plate inductor 188, of the oscillator. The l5 kc. signal induced in this coil 187 is supplied through a variable tapped resistor 189 and the tap 190 thereof to the high speed galvanometer 160 to furnish the driving energy therefor. By adjusting the position of the tap 190 along the resistor 189 the amount of energy supplied to the gavanometer 1611 can be varied to selectably adjust the oscillatory swing of the vibration mirror 159 (FIG. l2)

As a second output, the tuned plate oscillator 186 supplies, by a conventional coupling means, a 15 kc. signal to the control grid of a triode section 196 connected in a conventional manner as a frequency doubling amplilier circuit. The 30 kc. signal yielded by this triode sec- Considering now in more detail the polarized rectifier4 circuit 181, the heart of the circuit consists of atriode section 205 having a plate 206, cathode 207 and ,control grid 208 and another triode section 2Mb having a plate 211,

cathode 212, and control grid 213-, the two triode sections 205 and 210 being connected in reverse parallel relation in a loop circuit 21S. The other components of this loop circuit 215 consist of a resistor 216, a load 217 composed of two thyrite resistors 218-, 219 in series and the edge signal winding 100. in loop circuit 215, elements 216,

217 and 218 are in series with each other, with triode` sections 20S, 210 being connected (in the loop) to one end of resistor 2.16 and one end of edge signal winding 180.

It is evident that the 30 kc. second harmonic signal in duced in the edge signal winding E80k has a voltage which changes in direction for each half cycle. in the half cycle for which the edge signal voltage tends to force current around ythe loop circuit 2&5 in the clockwise direction, the triode section 2&5 will conduct current if the potential of its control grid 20S permits it to do so, but (resulting from its rectifying characteristic) the triode section 210 will not conduct irrespective ofl the potential on its control grid. Conversely, in the half cycle for which the edge signal voltage tends to force current around the loop circuit 21S in the counterclockwise direction, the triode section 210 will conduct if the potential on its control grid 213 permits it to do so, but the triode section 205 will not conduct irrespective of the potential on its control grid.

The control voltages for the two reverse parallel connected triode sections 205 and 2li) are respectively furnished by the control voltage windings 202 and 203, the Winding 202 being connected between the control grid 208 and cathode 207 of the triode section 205, while the winding 203 is connected between the control grid 213and the cathode 212 of the triode section 210. The two control voltage windings 202 and 203 are so respectivelyy coupled to the triode sections 205 and 210 that both windings furnish in phase control voltages to their respective triode sections.

With regard to the relations between the control voltages furnished to the triode sections 205, 210 by the control voltage windings 202, 203, Vand vthe edge signal voltages `furnished to these sections by the edge signal winding 180, it is evident that the 30 kc. signals induced in the control voltage windings are synchronously locked with the l5 kc. signal of the tuned plate oscillator E86. Moreover, the 30 kc. second harmonic signal induced in the edge signal winding 180 is also synchronously locked with the 15 kc. signal of the oscillator 186, by virtue of the cause and effect concatenation that this 30 kc.v signal 'is the second harmonic of the output signal of the edge photocel] 163, the photocell signal is generated by the oscillatory action of the vibration mirror 159', the mirror 159'is driven by the high speed galvanometer 160 and the driving energy for the galvanometer 16o is furnished from the l5 kc. oscillator. Hence, the control voltage signals in the windings V202, 203` and the edge signals in the winding 180 bear a synchronous relation to each other.

Assuming, however, that the signals oi the control windings establish a reference phase, the signal in the Yedge signal winding 180 may either have a voltage of reference phase, zero voltage, or a voltage 180 displaced l2 from reference phase, this latter condition being referred to hereafter as one of inverse phase. In FIGURE 13, the convention is adopted that, as to the edgel signal winding 180, a voltage of reference phase tends to drive current in the direction shown by the solid line arrow 225 While a voltage of inverse phase tends to drive current in the direction ofthe dotted line arrow 225. With respect to the plurality of possible edge signal phases, the various fact situations respectively causing the same will` be treated hereafter, it being necessary now to know only that different phase conditions are so produced.`

Over a full cycle of voltage alternation in the control voltage windings 202, 20'3, it is evident Vthat for a halt cycle thereof the grid-cathode bias of both triode sec tions 205, 210 will be negative, and that therefore, neither triode section can conduct, whatever thel phase of the edge signal voltage. For the remaining half cycle, howx bias forboth-triode sections 295 and 210; Vln this situa` ever, there will be a. simultaneous, positive, grid-cathode is in reference phase. (as shownby-the solid line arrow 225), the triode section 205 will conduce while the other triode section 210 remains non-conductive. As a result, current circulates clockwise around the loop circuitZflS to produce a positive voltage drop (as shown by the solid line arro-w 230) across the load 217. If,conversely, the voltage induced in the edge signal winding litl` is of inverse phase (as shown by the dotted line arrow 225'),`

the triode section 210 will conduct, while the other triode section 205 remains non-conductive. in this 'latter case, current circulates counterclockwise around the loop circuit 215 to cause a negative voltage drop (as shown by ythe dotted line arrow 230') across the load 2ll'7.V Of g course, in the situation where no voltage is induced in the edge signal winding 180, no current will circulate around the loop circuit 215 and no voltage will be generated across the load 217.

Since one or the other of the triode sections 265, 210 conducts, if at all, only during the positive half cycle for the control voltages, it is evident that the current caused to circulate around loop `circuit 215 assumes the iorrn of a set of similar polarity half cycles for an alternating Wave, the current half'cycles being of positive or negative polarity as to load 217 in vdependence on which one of triodes 205, 210` conducts. To smooth out the pulsations of this type of circulatory current, a condenser 235 is con- `nected in shunt across the series coupling of resistor 216 and load 217. The condenser 235 and the resistor, 2id

together serve to average out the pulsations inthe loop' circuit current to accordingly produce across thel load 217 f a smooth D.C. voltage, having respectively a positive and a negative polartiy in response to an edge signal of Y reference and inverse phase.

Considering the quantitative relation between the amplitude of the edge signal in winding and the amplitude of the voltage Vappearing across the load 217, the series connected thyrite resistors 218, 219 have a resistivity characteristic logarithmically related to the applied voltage. Since the voltage applied across resistor 2ll6` and `load 217v is substantially that of the edge signal, there may be` obtained the approximate expression:

V51-kill,

`where VL is the amplitude of the load voltage, Vp the harmoniccontrol voltage signals are respectively injected into the polarized rectifier circuit by means of transformers 179 and 201, it is evident that insofar as these two signal couplings are yconcerned the polarized rectifier 13 181 is completely free to float in potential. The rectifier circuit, however, is connected at the juncture of condenser 235 and thyrite resistor 219 to the cathode 240 of a triode section 241 connected as a conventionalcathode follower. The control grid 242 of triode section 241 receives, as an output of a triode section 243 (connected as a conventional D.C. amplifier) the image-carrying signal (FIG. 9) of the black color channel, the input of triode section 243 being supplied from limiter 45 (by the lead 46) with the invert of this signal. Thus from the cathode follower action triode section 241 the black image signal appears between cathode 240 and ground, causing the rectifier circuit 181 to exactly follow (as to the potentials of its internal circuits with respect to ground) the amplitude of the black image signal. Ac-

cordingly, the voltage with respect to ground appearing at the juncture of the resistor 216 and the thyrite resistor 218 represents, in voltage, the sum of the image-carrying black signal and the parallel edge correcting signal appearing across the load 217.

y The combined signal produced by the super position of the black image-carrying signal and the correction signal in the manner described is supplied to the input ofA a triode section 244 connected as a conventional phase inverting D.C. amplifier. From the output of triode section 244, the inverted combined signal is supplied to the control 'grid 245 of a triode section 246 connected in a conventional manner as a cathode follower. From the cathode 247 of this cathode follower triode section 246, the inverted combined signal representing the output of parallel edge detector circuits 47 (FIG. l) is supplied by the lead 48 to the black channel D C. amplifier 49.

Operation for Parallel Edge Correction By way of fuller explanation of the mode by which the pre-scanner optical system and parallel edge detector circuits restore the sharpness of parallel edges, reference is made to FIGURES 14a-18a, inclusive, 14b-18b, inclusive, and 14e-18e, inclusive. In these drawings, FIGURES 14a-18a are respectively associated with the solid line portions (designated by unprimed letters) or FIGURES 14e-18e, while FIGURES l4b-18b are respectively associated with the dotted line portions (designated by primed letters) of FIGURES 14C-18e.

FIGURES 14a-18a represent a portion of a visual subject 250 having thereon an edge 251 lying parallel to the scanning direction taken across the portion and forming a boundary between an upper light area 253 and a lower dark area 254. Viewing these figures in order from top to bottom, the visual subject portion 250 is traversed by a succession of horizontal scanning paths Z55-259, each path being traversed in a direction from lett to right, as shown by the arrow head 260. In each figure the scanning path traversing the same is displaced below the path of the figure above to give a direction of advance for'the scanning action as shown by the arrow 261. In vall the figures the solid line square 262 represents the part of the visual subject seen by the vibrating mirror 159 (FIG. l2) at the zero position for each sampling cycle thereof,

while the dotted line squares 263 and 264 represent the part of the visual subject 250 seen respectively for the maximum upward swing and maximum downward swing 0f the vibrating mirror 159. i

In FIGURES 14e-18e each of the figures shows three separate signals designated, respectively, as I, II and III, and representing, respectively, the output signal of edge detecting photocell 163, the second harmonic content of this signal, and the resulting signal across load 217 of polarized rectifier 181. For each of signals I, II, III the horizontal ordinate thereof represents distance taken along a horizontal scanning path, while the vertical ordinate thereof represents various signal amplitudes measured from respective base lines, each designated by the letters lTreating, the figures in detail, in FIGURE 14a the vibrating mirror 159'(FIG. 12) through each full cycle of .oscillation sees exclusively the light area 253. In consequence, the edge detecting photocell 163 (FIGS. l and 12) throughout a scan along path 255 receives constant light energy to produce a constant level output signal (FIG. 14C, wave form A). This constant level signal has zero second harmonic content (FIG. 14e, wave form B). Accordingly, the signal across load 217 of polarized rectifier 181 (FIG. 13) is of zero voltage (FIG. 14C, wave form C). y

In FIGURE 15a the scanning path 256 traversing the visual subject portion 250 has moved towards the dark area 254 to the extent where the vibrating mirror 159 for `a part of itsdownward swing views this dark area. For the interval for which the dark area 254 is seen, the light energy received by the edge detecting photo-cell 163 decreases. The photocell output signal for this interval, therefore, drops from its high, light tone level (FIG. 15C, Wave form D), the signal during the period of drop suhstantially following in form the 15 kc. sinusoidal wave which, through the galvanometer 160 (FIG. l2) drives the vibrating mirror 159. The photocell output signal, accordingly, has a wave form which is rich in a second harmonic component of the reference phase (FIGURE 15e, wave form E). This second harmonic-component is converted (as previously described) by the polarized rectifier 181 (FIG. 13) into a D.C. edge correcting signal of positive polarity across the load 217 thereof (FIG. 15e, Wave form F) for application, as described, to the main image-carrying signal (FIG. 9) to produce a Klight tone density peak 138 (FIG. 10).

In FIGURE 16a, the scanning path 257 taken across the visual subject 250 coincides with the parallel edge 251 upon that subject. In consequence, the vibrating mirror 159 during each complete sampling cycle sees equal amounts of the dark area 254 and the light area 253 to cause the edge detecting photocell 163 to produce an output signal symmetrical as to intervals in which the signal assumes light tone and dark tone levels (FIG. 16e, wave form G). As is well known, a signal of this sort has substantially no second harmonicy content (FIG. 16e, wave form H), and the polarized rectifier 181 (FIG. 13) accordingly produces across its load 2,17 a zero edge correcting signal output (FIG. 16C, wave form I). The situation shown by FIGURES 16a and 16C accordingly represents for the main image-carrying signal the center point for the transition line between light tone and dark tone levels 136 and 137" (FIG. 10).

In FIGURE 17a the scanning path 258V is so advanced that the vibrating mirror 159 over a sampling cycle sees the light area 253 only for a portion of its upward swing. For the interval for which this light area is thus seen, the light energy received by the edge detecting photocell 163 increases. Hence, for this interval the output signal fromthe vphotocell will rise upwards froma dark tone level (FIG. 17e, wave form I), the signal during the period of rise substantially following in form the l5 kc. driving signal for the vibrating mirror 159. The output signal of the photocell 163 accordingly will be rich in second harmonic component of the inverse phase (FIG. 17e, wave form K). This inverse phase second harmonic component is converted (as described) by the polarized rectifier 181 (FIG. 13) into a D.C. signal `of negative polarity (FIG. 17e, wave form L) for application ofv this latter signal to the main image-carrying signal (FIG. 9) t0 produce a dark tone density peak 139 (FIG. 10).

In FIGURE 18a the scanning path 259 has advanced to the extent where the vibrating mirror 159 during a full sampling cycle sees exclusively the dark area 254. The light energy received by the edge detecting phototube 163 will accordingly be low in amount and of constant value.

In consequence, the photocell output signal will be a constant low dark tone level (FIG. 18C, wave form M), the signal having zero second harmonic content (FIG. 18e, Wave form N). It follows in this case that the polarized Aportion and the length s1 of the light `tone portion.

rectifier 181 (FIG. 13) produces zero edge correcting signal across its load 217 (FIG. 18C, wave form O).

FIGURES l4bl8b, inclusive, are respectively analogous as to subject matter with FIGURES l4a-18a, each feature in the l-atter group of figures being identified by the primed designation Vof the counterpart feature in the former group of figures. The principal distinction between the two groups of figures is that in FIGURES 14b-l8b the scanning paths 255-259 in traversing the visual subject portion 250' advance from a dark area 254' to a light .area 253. With this latter type of advance signals will be derived characterized by the dotted line wave forms of FIGURES 14e-18C. In view of the foregoing discussion, the significance of these wave forms are, for the most part, self-evident. Of note, however, is the fact that, in contrast to the situations shown by FIGURES 15a and l7a,-where there are respectively produced, second harmonic signals of reference phase (FIG. 15C, wave form E) and inverse phase (FIG. 17C, wave form K) the situations shown by FIGURES 15b `and l7b, respectively, produce 1 second harmonic signals of inverse phase (FIG. 15C, Vwave form E) and'reference phase (FIG. 17C, wave :form K). It follows that in the separate ycases of light to dark scan advance and dark to light scan advance, the time occurrence of the positive and negative polarity edge correcting signals isv reversed. (Compare FIG. 15e, wave forms F and F and FIG. 17e, waveforms L and L.) As a matter of space occurrence, however, in both cases the proper edge correcting signals are obtained lsince in both cases there is applied to the image-carrying signal (FIG. 10) a light tone correction 138, between the transition line 135" (representing the edge) and the light tone leve] proper 136", and a dark tone correction 139 between the transition line 135 and the dark tone level proper 137".

It should alsok be noted that the pre-scanner optical system and the polarized rectifier 181 operate to produce the proper edge correcting signals, whether there is right -hand or leftscan advance. FIGURES 14a-18a and 14hlSb show right hand scan advance, the direction of advance from one scanning path to the next being right handed with respect to the travel direction along each scanning path. Left hand scan advance from a vdark to a Y edge, for any given sampling cycle of mirror 159, the

amplitude of the signal across load 217 (excluding from consideration the compression effect of Vthyrite resistors 21S, 219), may be approximately determined by the exwhere A is the signal amplitude, s the length (transverse to the scanning path) of the strip of visual subject seen by mirror 159, sd and s1 the respective transverse lengths of the dark Vand light tone portions seen in the whole length s ofthe mentioned strip, td and' t] the average tone densities of the dark and llight tone portions, g the signalgain factor between the light receiv ing input of edge phototube 163 and the output of the parallel edge circuits 47, and K is a constant.

In the expression above set forth the term sd-sl represents the comparative dominance for the length s of the whole strip between the length sd of the dark tone sd lis less than s1, so that the light tone portion dominates,v

the dark, then the sine function (enclosed in the above expression) will have a positive value preducing'a positive amplitude (or highlevel for the sfignal). If sd equals s1, so that the dark and light tone'por- .tions are evenly balanced, with no dominance of one or the other, then the sine function will have a value of zero yielding zero signal amplitude. Finally, if sd `is greater than s1, so that the dark tone portion dominates the light,`then the sine function will have a negative value, producing a negative polarity (or'low level) for the amplitude of the signal. Thus'the amplitude and polartiy of the signal across load 217 (or, equivalently, Wtlie level manifested thereby) depends primarily upon which one of two relatively light and dark tone portions inthe length of strip scanned by mirror l159 dominatesV the other portion. Y

In the expression above set forth the term td-tl represents the contrast between the average tone densities `of the light tone and dark tone portions detected. As will be seen, the amplitude of the signal varies directly with the tone density contrast present. Also, it will be seen that in the expression above set forth thesignal 1 amplitude A varies directly with the signal gain factorl present. Over the expected range of tone density contrast, therefore, the desired amount of edge-accentuating effect may be produced by preselecting, through adjust-v ment of the plate voltage on phototube 163, the value of signal gain which is appropriate.

yAs stated, the output signal of parallel edge circuits 47 represents in the inverse from the black image-carry ing signal superposed (in the presence of a parallel edge) with an appropriate paralltl edge correcting signal. This inverted combined signal is supplied by lead 48 (FIG. 1) to the control grid 122 of triode section 123 in black D.C. amplifier stage 49. In passing through amplifier 49, the signal on grid 122 is re-,inverted to appear on the output lead 5l) of amplier stage 49 as an upright cornbined signal (dotted line graph o f FIG. l0) character- It will be re` ized by restored parallel edge sharpness. K called that (as hitherto described) by virtue of the transverse edge correcting signal supplied to control grid 1,22 by lead 120, the signal on output lead'50 is also characterized by restored transverse edge sharpness. :Hence the signal on lead Sti actuates black glow lamp 51 to expose a black half-tone separation characterized by both restored transverse and restored parallel edge sharpness.

It will be understood that by combining the transverse and parallel edge correcting signals in the mode described, proper edge correction is obtained whether the edge scanned is truly transverse, truly parallel or is (as 4is `:more often the case) a skewed edge having transverse` and parallel edge components. Moreover, in `view of the Y fact sharpness for any orientation of the :scanned edge,

it is apparent that proper edge correction is attained whether the edge is of straight line or of other coniiguration.

With regard to this combining together of transverse land parallel edge correcting signals, there may haveal- Y ready been noted in the foregoing discussioncertain aspects commonly characterizing both the means for obtaining transverse edgecorrection and the means for obtaining parallel edge correction. That each type ofedge.

ledges, assume thatthe edge correcting effect .takes place with regard `to apshort length of edge. In .the transverse case the edge of short length may be thought fto :be .a .Patrios eftbaetse .519 i951@ 2 Whrhfis .traversed in brackets 17` by the scanning aperture 56. In the parallel case` the edge of short length may be thought to be a portion of the edge 126 in FIG. 8 which underlies the scanning aperture 129 when the same views the edge 126 at the line 130a.

If the edge is transverse to the scanning direction (FIG. 2), the scanning aperture crosses the short length of edge by its movement in a single scanning path. If the edge is parallel to the scanning direction (FIG. 8), the scanning aperture crosses the short length of edge by an advance of the scanning paths in the direction of arrow 130 such that the aperture for at least one scan views a portion of the visual subject which contains the short length of edge. In either case, however, the progress of the aperture in crossing the edge is such that the aperture views first an area of aperture size to one side of the length of edge, then a similar size area including the length of edge, and finally a similar size area to the other size of the length of edge. The image signals derived from these separate areas will represent the edge as a change in signal level over time. However, the image signal which is produced from each aperture size area represents an unresolved mixture of light from the details within each area, of particular interest being the one or more unresolved light mixtures derived both from the length of edge itself and from `other details within the one or more edge-containing, aperture size areas Hence, as the aperture crosses the edge by progressing, one after another, through the aperture size areas, the change in level of the image signals from the areas will be (as more fully discussed heretofore) a gradual change in level which is not a satisfactory electrical representation of the tone density transition of the edge.

Whether in the transverse edge or parallel edge case, the loss in sharpness of the edge as electrically represented is corrected for by utilizing a sensing system which, in the course of progress of the aperture through the mentioned areas, senses the presence of length of edge to develop sharpening signals'which vary in signal level over time as the inverted second differential of the change in image signal level over time. In the transverse edge case, the significant part of the sensing system which is effective is comprised essentially of the differential circuits 96 and 1104 (FIG. l), while in the parallel edge case, the part of the sensing system whichiseiective is comprised of the optical apparatus of FIG. 12 and the electrical apparatus of FlG. 13. The inverted second differential change in signal level is represented in the transverse edge case by the wave form of FIG. 6f, and in the parallel case by the difference in amplitudes between the solid and dotted graph lines of FIG. l0. In either case, the sharpening signals developed by the subsystem areV added to the image signals developed by the electrooptical scanning unit to give an improved electrical representation of the sharp tone density transition of the length of edge.

While the basic mode for obtaining edge correction has been limited in the description above to refer to pure transverse or parallel edges only, the principles involved pertain equally well to edges at skew angles-to a scanning direction or to a direction of scanning advance. Hence, it will be seen that the described basic manner of edge correction attainment is by its nature of general appli-V cation to edges of any orientation upon a visual subject.

Ordinarily, to attain the desired restoration of parallel edge sharpness, it is not necessary to apply the parallel edge correcting signal to any color channel other than the black. This fact obtains for the reason that in the manufacture of color print from a set of color separations, the black separation dominates the others in determining, for a viewer, the visual appearance of the color print. Thus to the eye the edge sharpness of the black separation may be made sufficient to compensate for the loss of edge sharpness in the other color channels, while at the same time the problem is avoided of registering 18 sharp edges in all four color separations. For applica-4 tions where desirable, however, an appropriate amount of parallel edge correcting signal may be supplied to one or more of the' color channels in the same mode as hitherto described for the black channel.

The High Speed Galvanometer Turning now to the structure of the high speed galvanometer 166 (FIG. l2), as shown in FIGURES 19 and 20 a pair of magnetically conducting, longitudinal yoke bars 260 and 261 spaced apart from each other in opposite parallel relation, are adjustable towards and away from each other by a conventional supporting and adjusting means (not shown). Means is provided for inducing magnetic flux of opposite polarity in the two yoke bars. For example, the two yoke bars by adjustment towards each other may be adapted to clamp between themselves a transversely extending permanent magnet 262 (made, for example, from Alnico) having a north pole proximate the yoke bar 26u andY a south pole proximate the yoke bar 261.

The two yoke bars, at corresponding ends thereof, respectively support north and south pole pieces 264 and 265 in such relation that the two pole pieces extend transversely towards each other. Both the pole piece 264 and the pole piece 265 are adjustable in transverse extension by means of respective set screws 266, 267, passing through respective open slots 26S, 269 in the outer faces of the pole pieces 264,' 265 to enter (in threaded relation) respective holes270, 271 formed in the ends of the yoke bars.

The` two pole pieces 264, 265 are characterized by respective bifurcations 272, 273 at intermediate extension positions for the pole pieces, the bifurcation 272 dividing the pole piece into an upper finger 274 and a lower finger 276, and the bifurcation 27.3 similarly dividing the pole piece into an upper finger 275 (FIG. 19) and a lower finger 277. Y

lConsidering the pole rpiece 264, the upper finger 274 thereof assumes a hook-like form, the surface 278 of the finger, 'as seen in FIGURE 20, curving away rearwardly in transverse extension to keep at a distance the longitudinal center line 28) of the galvanometer assembly. When transversely beyond this center line 280 the surface 278 curves forwardly, in continued spaced relation from the center line, to form, as a termination of the finger 276, a north pole tip 282 for this upper finger.

The upper finger 275 (FIG. 19) is radially symmetrical with upper finger 274 as to center line 280. Upper finger 275 curving around the centerline on the side opposite from that dened by finger 274. The upper finger 275 terminates in a pole tip 283 disposed in spaced apart and transversely opposite relation from the pole tip 282.

The lower fingers 276 and 277 of the pole pieces 264 and 265 linearly extend transversely towards each other to form at their near extremities respective pole tips 284 and 285. Moreover, pole tip 284 is disposed to directly underlie upper pole tip 283 while lower' pole tip 285 is disposed to directly underlie upper pole tip 282. The longitudinally matched pair of pole tips 283, 284 establish between them a magnetic field running from north charged pole tip 284 to south charged pole tip 283 while the longitudinally matched pair of pole tips 282, 285 establish a magnetic eld running from north charged pole tip 282 to south charged pole tip 285. The two magnetic fields so established are thus relatively reversed in direction.

In centrally spaced relation between the lower pole tips 284, 285 there is disposed one end portion 290 of a laminated stem 291 aligned with the center line 280 of the assembly. The end portion 290 is adapted to be gripped by a pair of blocks 292, 293 composed of semiyieldable material (as, for example, plastic resin), the blocks 292, 293 being respectively positioned between the end portion and the lower fingers 276, 277. By adjusting the pole pieces 264, 26:? towards each other and thereafter clamping both in place, the two blocks 292, 293 are caused to clamp therebetween the end portion 290. The stem 291 is formed of four longitudinally extending, stacked, at larninations 295, 296, 207' and 298. As to these four stem components, the two inner laminations 296, 297 at end portion 290 project linearly beyond the two outer laminations 295, 298 to a point of equidistance between they upper and lower ngers of each pole piece, the projecting portions of laminations 296, 297 forming respectively the flex sections 300, 301. At this point of equidistance the two inner laminations 296, 297 assume right-angle bends to form respectively a pair of mutually diverging, transversely extending, wings 302, 303. Wing 302 is suiiciently long that the extremity thereof lies equidistantly between pole tips 283 and 284 while the extremity of wing 303 is similarly positioned between pole tips 202 and 20S.

The wings 302, 303 form together a magnetic armak ture 305 the motion of which is adapted to drive the vibrating mirror 159. Mirror 159 is affixed in a conventional manner (as by soldering, for example) to the j upper sides ofwings 302, 303, the rigidity of mirror 159 imparting rigidity to armature 305 along substantially its whole extension.

Driving energy for armature 30S is supplied by an exciting coil 306 encircling the stem 291 and carrying current derived through tap 190 (FIG. 13) from the 15 kc. signal of the oscillator 106.

In operation the l kc. signal, in passing through the coil 306, induces in the laminations of the stem 291 a magnetic ilux alternating as to polarity at the frequency of the signal. The alternating flux so created causes both ends of armature 305 to simultaneously change magnetic polarity at a l5 kc. rate. The two endsof armature 305, however, are respectively disposed in permanent magnetic fields of opposite direction. In consequence a y kc. alternating torque is exerted in the armature 305..

Since the resilience of ilex sections 300, 301 permits armature movement to a limited extent, the armature 305 responsive to the torque exerted on it will sinusoidally oscillate in the space between the upper and lower pole tips. Mirror 159 will accordingly be driven at a 15 kc. rate to perform its previously described function in the pre-scanner optical system (FIG. l2).

For the purpose of obtaining maximum driving action from the armature 30S, it is advantageous to bring the mass of the flex sections 300, 301, Wings 302, 303, and

mirror 159, and the resilience of flex sections 300, 301y into mechanically resonant relation at the frequency of the 15 kc. galvanometer driving signal. Tuning for mechanical resonance may be accomplished through ad justment ofthe length of the flex sections 300, 301 by sliding (prior to clamping of stem 291 into the assembly) the inner laminations 296, 297 longitudinally to thereby change the relative positions thereof with respect tothe outer laminations 295, 298. When the relative position yielding mechanical resonance at the l5 kc. driving frequency has been reached, the inner and outer laminations are fixed in this relative position by appiying a conventional clamp member 31S to the stem 291 to bind together the component laminations.

The galvanometer construction just described is highiy advantageous in that by virtue of the structure thereof a relatively large sized mirror (for example, a square mirror Ms inch on the side) may be oscillated at a rate of at least l5 kc. Such high speed oscillation is necessary iu a parallel edge correction system to obtain (as described) adequate sampling of a visual subject to either side of a scanning path taken across the subject.

Ortho-Luminous Edge Correction Reverting to the'electronic printer of FiGURE 1, in ordinary practice the relative amplitude of the various transverse edge correcting signals are adjusted by conventional means (not shown) so that the amplitude of the is desirable, since (as explained) a black color separation of pronounced edge sharpness, when combined with other less sharp color separations to form a color print, will give an adequate visual impression of edge-sharpness to the color print as a whole. At the same time, the problem of ,registering sharp edges in all `four separations is avoided. To avoid registering diticulties, it may, in fact, upon occasion, be desirable to attain all transverse edge sharpness correction through the black channel,` the amplitude of the edge correcting currents in the color channels being reduced to zero.

Where the electronic printer circuits are adjusted to obtain transverse edge sharpness predominantly by means of the black channel, andl a single color channelV (.e'g., magenta) is employed to supply the black' channel with the correcting signal, the single color channel may, on occasion, not furnish a sufficient amount of signal to the black to give the desired amount of edge restoration. For example, where, as in FIGURE l, the black channel edge correcting signal is derived over lead 120 from the magenta color channel, and it happens that the areas bounding a scanned edge produce only a weak magenta imagecarrying signal, the signal fed over lead 120 may not beV sufficiently strong to give the desired edge. correctingV effect.

in FIGURE 21, there is shown a modification of the electronic printer circuits, in which, for a scanned edge adjoining an area of any color, it is assured that the proper Y amount of edge correcting signal is supplied to the black channel. :In the modiiication shown, theV edge correcting signal on lead 113' of the magenta channel is coupled to control grid 122 of triode section 123 in black D.C. amplifier stage 49 by the series connection of lead 120, conf denser 1121 (the circuitl to this point being similar to that of FlGURE l), and a resistor 323 of 1.8 megohms value. The yellow channel edge correcting signal is coupled from lead 113 to control grid 122 by the series connection of lead 321, condenser 322, and resistor 320 of 30 megohms value. The cyan channel edge correcting signal is coupled from lead 113 to control grid 122 by the series connection of lead 324, condenser 325 and 323 and 326 have graded resistance values causing proportional attenuation of the signals passing therethrough,

Y in edge correcting effect the magenta channel influence exceeds the cyan channel influence. so given to the edge correcting signals from the various color channels for the reason that to the human eye the presence of an edge is least apparent where the edge bounds a bright colored area (e.g., yellow) and most apparent where the edge bounds a darkl colored area (e.g., magenta); Hence, with regard to edge sharpness, in order for a replica to appear to the eye as a. true reproduction of theV original visual subject, it is necessary that the collectiveV transverse edge correction effect of the three color channels be in ortho-luminous relation, viz. that when different edges adjoining variously colored edges of the visualsubject. The relative resistance values of lresistors* 320, 323 and 326 are,- in FIGURE' 2l', prop- Unequal Weight is El erly proportioned to yield this ortho-luminous relation between the three edge correcting signals respectively supplied from the yellow, magenta.l and cyan color channels.

The specific embodiments shown in the drawings and described in the specification are obviously susceptible of modification within the spirit cf the invention. A wide range of equivalent elements will occur to those skilled in the art in place of the various components of the systems disclosed herein. The specific embodiments described, therefore, are to be regarded merely as illustrative and not as restricting the scope of the following claims.

I claim:

l. A mirror galvanometer comprising, a magnetic structure defining two air gaps spaced apart in a dimension, means for sustaining in said gaps fixed magnetic fields respectively running in opposite directions normal to said dimension, a pair of extended fiat-faced members of resilient magnetically conductive material with right angle bends therein on bend lines transverse to the extensions thereof, said members being disposed in -backto-back relation to form a T-configuration with a cross arm and a shank, a mirror atiixed to both said members along said cross arm to impart rigidity thereto, means to damp the shank of said T-configuration at an adjustable length from said cross arm to provide flex sections between said damping means and cross arm, means for holding said T-contiguration relatively fixed with said structure, said T-coniiguration having its shank aligned transverse to said dimension in the plane defined by said dimension and said directions, and having separate cross arm portions of said members in said two respective gaps, and means for inducing an alternating polarity magnetic charge in said cross arm. y

2. A mirror galvanometer assembly comprising, a pair of spaced pole pieces, a pair of fingers extending respectively from said pieces to terminate in a pair of first pole tips therefor, said tips being spaced apart in a dimension, another pair of fingers respectively extending from ones of said pieces to terminate in a pair of second pole tips therefor, each second pole tip being spaced from the first pole tip of the other pole piece in one direction normal to said dimension, all of said pole tips forming together two pairs of matched first and second pole tips with air gaps therebetween, means for inducing magnetic flux in said pieces and lingers to cause opposite polarity fixed magnetic charges in pole tips for different pole pieces, a pair of extended fiat-faced members of resilient magnetically conductive material with right angle bends therein on bend lines transverse to the extensions thereof, said members being disposed in back-to-back relation to form a T-configuration with a cross arm and a shank, a mirror affixed to bothsaid members along said cross arm to impart rigidity thereto, meansto damp the shank of said T-conguration at an adjustable length from said cross arm to provide ex sections between said damping means and cross arm, means relatively fixing the disposition of said T-coniiguration with said pole pieces, ngers and pole tips, said T-configuration in said disposition having the shank thereof aligned transverse to said dimension in the plane defined by said dimension and said directions, and having separate cross arm portions of said members respectively disposed in said gaps, and means for inducing an alternating polarity magnetic charge in said cross arm.

3. Apparatus comprising, a horizontal armature member having first and second separated portions and supported centrally of said portions to be tiltably movable in a vertical plane, a first pole piece having a pair of pole'tips disposed in said plane over and under, respectively, said first and second portions, a second pole piece having a pair of pole tips disposed in said plane under and over, respectively, said first and second portions to form a pair of air gaps with the pole tips of said first piece, means to impart opposite unchanging polarity magnetic charges to said pole pieces to thereby produce oppositely directed magnetic fields in said two air gaps, and winding means magnetically coupled with said member and vresponsive to an electric current signal applied thereto to'impart a magnetic charge of the same magnetic polarity to each of said portions of said member, said charge and said fields being adapted together to produce torque on said member.

References Cited in the file of this patent UNITED STATES PATENTS 1,573,739 ONeill Feb. 16, 1926 ,1,637,442 Dorsey Aug. 2, 1927 1,930,677 Floyd Oct. 17, 1933 1,932,520 Horsch Oct. 3l, 1933 2,059,159 Whitaker Oct. 27, 1936 2,127,427 Scheldorf Aug. 16, 1938 2,163,195 Edwards June 20, 1939 2,432,424 Hyland Dec. 9, 1947 2,454,425 Bauer Nov. 23, 1948 FOREIGN PATENTS 823,527 Germany Dec. 3, 1951 UNITED STATES PATENT OFFICE CERTIFICATE OF CORRECTION Patent. No. 3,029,381 A April 1o, 1962 William West Moe It ia hereby certified that error appears in the above numbered patent requiring correction and that the said Letters Patent should read as corrected below.

g Column 51u line 58, for "paritcularly" read particulrly -s-,g line 6'?, for "illustration" read illusion --3 column 1D, line 68, for "gavanometer" read galvanometerg column 13, line 52, for lett" read left --5 column l5q line 38, after "left" insert hand column lo,z line 32., for "paralltl" read parallel --5 line 53, after "fact" insert that the edge correction system described restores edge Signed and sealed this 24th day ojJuly 1962.`

(SEAL) Attest:

ERNEST w. swlnER DAVID L. LADD Atteeting Officer Commissioner of Patents 

